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lons of different momentum (p), having t...

lons of different momentum (p), having the same charge, enter normally a uniform magnetic field. The radius of the orbit of an ion is proportional to

A

`P`

B

`1/p`

C

`P^2`

D

`1/p^2`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the relationship between the radius of the orbit of an ion moving in a magnetic field and its momentum, given that the ions have the same charge. ### Step-by-Step Solution: 1. **Understanding the Motion of Charged Particles in a Magnetic Field**: When a charged particle moves in a magnetic field, it experiences a magnetic force that acts perpendicular to both the velocity of the particle and the magnetic field. This force causes the particle to move in a circular path. 2. **Expression for Magnetic Force**: The magnetic force \( F \) acting on a charged particle moving with velocity \( v \) in a magnetic field \( B \) is given by: \[ F = qvB \] where \( q \) is the charge of the particle. 3. **Centripetal Force**: For a particle moving in a circular path of radius \( r \), the centripetal force required to keep it in that path is provided by the magnetic force: \[ F = \frac{mv^2}{r} \] where \( m \) is the mass of the particle. 4. **Equating the Forces**: Since the magnetic force provides the centripetal force, we can set the two expressions equal to each other: \[ qvB = \frac{mv^2}{r} \] 5. **Rearranging the Equation**: Rearranging the equation to solve for the radius \( r \): \[ r = \frac{mv}{qB} \] 6. **Substituting Momentum**: The momentum \( p \) of the particle is defined as: \[ p = mv \] Therefore, we can substitute \( mv \) in the radius equation: \[ r = \frac{p}{qB} \] 7. **Proportionality**: Since the charge \( q \) and the magnetic field \( B \) are constants (as given in the problem that the ions have the same charge), we can conclude that the radius \( r \) is directly proportional to the momentum \( p \): \[ r \propto p \] ### Conclusion: The radius of the orbit of an ion in a magnetic field is directly proportional to its momentum.
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